2018
DOI: 10.1002/smll.201704429
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High‐Responsivity Photodetection by a Self‐Catalyzed Phase‐Pure p‐GaAs Nanowire

Abstract: Defects are detrimental for optoelectronics devices, such as stacking faults can form carrier-transportation barriers, and foreign impurities (Au) with deep-energy levels can form carrier traps and nonradiative recombination centers. Here, self-catalyzed p-type GaAs nanowires (NWs) with a pure zinc blende (ZB) structure are first developed, and then a photodetector made from these NWs is fabricated. Due to the absence of stacking faults and suppression of large amount of defects with deep energy levels, the ph… Show more

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Cited by 61 publications
(47 citation statements)
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References 63 publications
(175 reference statements)
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“…(NWs) represent a promising platform to implement quantum computation and quantum information processing [1,2] and this specific implementation, NWs, provides a versatile material system to demonstrate innovative nanoscale devices, such as lasers, photo-sensors and solar cells [3][4][5][6][7][8][9]. In this frame, compared to other semiconductor NW systems, InP NWs display a lower susceptibility to non-radiative surface states and a stronger photoluminescence (PL) emission: this material system is therefore of particular interest for quantum-photonics application [10][11][12][13][14][15][16][17].…”
mentioning
confidence: 99%
“…(NWs) represent a promising platform to implement quantum computation and quantum information processing [1,2] and this specific implementation, NWs, provides a versatile material system to demonstrate innovative nanoscale devices, such as lasers, photo-sensors and solar cells [3][4][5][6][7][8][9]. In this frame, compared to other semiconductor NW systems, InP NWs display a lower susceptibility to non-radiative surface states and a stronger photoluminescence (PL) emission: this material system is therefore of particular interest for quantum-photonics application [10][11][12][13][14][15][16][17].…”
mentioning
confidence: 99%
“…Due to the accumulated photon-generated holes on the NW surface, electrons move to the surface through tunneling, and crossing the barrier will recombine at the surface, leading to a weaker interband emission but longer emission wavelengths. The p-type GaAs NW has shown extraordinary photoelectric properties in photoelectric detection [ 139 ]. The surface state of the p-type NW is similar to that of the donor and can trap holes, leading to the negatively charged surface depletion zones and the downward bending of the CB and VB bands ( Figure 12 c).…”
Section: Structural–dependent–physical Properties Of Iii–v Nwsmentioning
confidence: 99%
“…The main part of doping studies currently exists for Au or Ga seeded GaAs NWs [54][55][56][57][58][59]. The most commonly used n-type dopants are Te [55,57,60] and Si [61][62][63], while the most commonly used p-type dopants are Be [55,58,59,64], C [61], and Zn [54,56,57]. During the doped NW growth, the decomposition and diffusion of different growth species in the vapor phase on the surface of the NW and in the catalytic particles will affect the homogeneity of carrier concentration, material composition, and doping profile abruptness.…”
Section: Doping In Gaas Nwsmentioning
confidence: 99%